To determine the RMS value of the induced current in the ring, we need to follow a series of logical steps and calculations involving electromagnetic induction concepts.
- The solenoid has a time-varying current \( i(t) = 10 \sin(\omega t) \) where \( \omega = 1000 \) rad/s.
- The number of turns per unit length of the solenoid is given as \( n = 500 \, \text{turns/m} \).
- The radius of the ring is \( r = 1 \, \text{cm} = 0.01 \, \text{m} \) and its resistance is \( R = 10 \, \Omega \).
- We use Faraday's Law of electromagnetic induction to find the induced EMF \( \mathcal{E} \) in the ring. The magnetic field inside a solenoid is given by \( B = \mu_0 n i \), where \( \mu_0 = 4\pi \times 10^{-7} \, \text{T} \cdot \text{m/A} \) is the permeability of free space.
- The magnetic flux through the ring is \( \Phi = B \cdot \pi r^2 = \mu_0 n i \pi r^2 \).
- The induced EMF in the ring by Faraday's Law is:
\[\mathcal{E} = -\frac{d\Phi}{dt} = -\pi r^2 \mu_0 n \frac{di}{dt}\]- Substitute \( i = 10 \sin(\omega t) \), then:
\[\frac{di}{dt} = 10\omega \cos(\omega t)\]- Thus, the induced EMF becomes:
\[\mathcal{E} = -\pi r^2 \mu_0 n \times 10\omega \cos(\omega t)\]- The magnitude of the instantaneous EMF is:
\[\mathcal{E}_0 = \pi (0.01)^2 \times 4\pi \times 10^{-7} \times 500 \times 1000 \times 10\]Calculate the above expression to find \( \mathcal{E}_0 \):
\[\mathcal{E}_0 = \pi \cdot 0.0001 \cdot 4\pi \cdot 10^{-7} \cdot 500 \cdot 10^4 \approx 2 \times 10^{-3} \, \text{V}\]- The RMS value of the current \( I_{\text{rms}} = \frac{\mathcal{E}_0}{\sqrt{2} R} \) due to the sinusoidal nature of the induced EMF. So:
\[I_{\text{rms}} = \frac{2 \times 10^{-3}}{\sqrt{2} \cdot 10} = \sqrt{2} \times 10^{-4} \, \text{A}\]Thus, the RMS value of the induced current in the ring is \( \sqrt{2} \times 10^{-4} \, \text{A} \), which matches the correct answer.